| 摘要 |
<p>1,251,557. Lasers. COMMISSARIAT A L'ENERGIE ATOMIQUE. 21 Feb., 1969 [12 March 1968], No. 9448/68. Heading H1C. An output pulse from a laser generator is amplified in a further laser by using a beam splitter to separate the pulse into two pulses a and b, the pulse a being subjected to an optical path delay while the pulse b is amplified in the further laser, and the amplified pulse b being then subjected to the same optical path delay while the pulse a is amplified, the two pulses being finally recombined. In this manner the intensity of the generator output pulse is reduced so as to avoid thermal damage to the amplifier laser rod. As shown in Fig. 1, the laser generator comprises a laser rod 1, partially transmitting mirror 3 and a rotating Q-switching prism 2, the output pulse being vertically polarized at 4 before pulse division takes place at a beam splitter 5. The transmitted pulse b is passed through Glan prisms 6 and 12 and laser amplifying rods 10, 11, without effect on the vertical polarization, the second Glan prism 12 being crossed with respect to prism 6 that the pulse b is diverted into an optical delay path formed by mirrors 13 and 14. The pulse a is deflected by the beam splitter 5 into an optical delay path comprising mirrors 7, 8 before passing through the laser rods 10, 11 and Glan prism 12, its vertical polarization being converted to horizontal polarization by a Fresnel prism or ¢ wave plate 9 so that reflection takes place at prism 66. The two pulses a and b, which are respectively transmitted and reflected by prism 12, are focused on to a common spatial point F by lenses 15, 16. In a modification, Fig. 2, the two pulses a and b are passed through the laser amplifier rods in opposite directions, the initially delayed pulse a being reversed in direction by the optical path delay formed by mirrors 18, 19, 20 and the polarization-changing Fresnel prism 9.</p> |
